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<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0" article-type="research-article"><?xmltex \makeatother\@nolinetrue\makeatletter?><?xmltex \hack{\hyphenation{methods}}?><?xmltex \hack{\hyphenation{result}}?><?xmltex \hack{\hyphenation{Gra-velle}}?><?xmltex \hack{\hyphenation{measurement}}?>
  <front>
    <journal-meta><journal-id journal-id-type="publisher">NHESS</journal-id><journal-title-group>
    <journal-title>Natural Hazards and Earth System Sciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">NHESS</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Nat. Hazards Earth Syst. Sci.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1684-9981</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/nhess-23-415-2023</article-id><title-group><article-title>Detecting anomalous sea-level states in North Sea tide gauge data using an autoassociative neural network</article-title><alt-title>Neural networks detect anomalous sea-level states</alt-title>
      </title-group><?xmltex \runningtitle{Neural networks detect anomalous sea-level states}?><?xmltex \runningauthor{K. Wahle et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Wahle</surname><given-names>Kathrin</given-names></name>
          <email>kathrin.wahle@hereon.de</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2 aff3">
          <name><surname>Stanev</surname><given-names>Emil V.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Staneva</surname><given-names>Joanna</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-4553-392X</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Helmholtz Zentrum Hereon, Geesthacht, Germany</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Research Department, University of Sofia “St. Kliment Ohridski”,
Sofia, Bulgaria</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Meteorology and Geophysics, University of Sofia “St.
Kliment Ohridski”, Sofia, Bulgaria</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Kathrin Wahle (kathrin.wahle@hereon.de)</corresp></author-notes><pub-date><day>2</day><month>February</month><year>2023</year></pub-date>
      
      <volume>23</volume>
      <issue>2</issue>
      <fpage>415</fpage><lpage>428</lpage>
      <history>
        <date date-type="received"><day>24</day><month>June</month><year>2022</year></date>
           <date date-type="rev-request"><day>29</day><month>June</month><year>2022</year></date>
           <date date-type="rev-recd"><day>8</day><month>November</month><year>2022</year></date>
           <date date-type="accepted"><day>29</day><month>December</month><year>2022</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2023 Kathrin Wahle et al.</copyright-statement>
        <copyright-year>2023</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023.html">This article is available from https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023.html</self-uri><self-uri xlink:href="https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023.pdf">The full text article is available as a PDF file from https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e116">The sea level in the North Sea is densely monitored by tide gauges. The data they provide can be used to solve different scientific and practical
problems, including the validation of numerical models and the detection of extreme events. This study focuses on the detection of sea-level states with anomalous spatial correlations using autoassociative neural networks
(AANNs), trained with different sets of observation- and model-based data.
Such sea-level configurations are related to nonlinear ocean dynamics;
therefore, neural networks appear to be the right candidate for their
identification. The proposed network can be used to accurately detect such
anomalies and localize them. We demonstrate that the atmospheric conditions
under which anomalous sea-level states occur are characterized by high wind
tendencies and pressure anomalies. The results show the potential of AANNs
for accurately detecting the occurrence of such events. We show that the
method works with AANNs trained on tide gauge records as well as with AANN
trained with model-based sea surface height outputs. The latter can be used
to enhance the representation of anomalous sea-level events in ocean models. Quantitative analysis of such states may help assess and improve numerical model quality in the future as well as provide new insights into the nonlinear processes involved. This method has the advantage of being easily applicable to any tide gauge array without preprocessing the data or
acquiring any additional information.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

      <?xmltex \hack{\break}?>
<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e130">The dynamics of sea level in tidal basins are one of the most addressed topics in physical oceanography. Theoretical prediction of tidal motion was pioneered by the application of a Fourier analysis by Lord Kelvin (Thomson, 1880) and later improved by Doodson (1921), who developed the
tide-generating potential in harmonic form. Analysis and interpretation of tidal observations by Proudman and Doodson (1924) enhanced the understanding
of sea-level fluctuations due to winds and changes in atmospheric pressure.
The development of numerical 2D storm surge models by Peeck et al. (1983)
and Flather and Proctor (1983) led to early warning systems for coastal
flooding. With increasing computational power and the availability of
satellite data, sea-level predictions have been continuously improved.
However, current model predictions are not always perfect (Stanev et al., 2015a; Sandery and Sakov, 2017; Staneva et al., 2016; Ponte et al., 2019; De Mey-Frémaux et al., 2019; Jacobs et al., 2021), which emphasizes the need for further
understanding of sea level.</p>
      <p id="d1e133">A recent important evolution in predicting sea level in the North Sea was
achieved in the framework of the development of the northwest European shelf
forecasting system (e.g., O'Dea et al., 2012; Tonani et al., 2019) by enhancing the model resolution to 1.5 km. Thus, dynamical features such as
coastal currents, fronts, and mesoscale eddies are better resolved, and the
model results are improved, especially when compared to high
spatial–temporal resolution observations.</p>
      <p id="d1e136">Satellite altimetry has added critical information in the last 30 years
(Madsen et al., 2015). Notably, different<?pagebreak page416?> measurement techniques have
different advantages and disadvantages. Satellite-derived sea-level information, which has revolutionized oceanography and climate science,
particularly in addressing global and large-scale change, is of limited use
when addressing near-coastal short-periodic variability. However,
advancements are underway, and new satellite missions characterized by
better spatial and temporal sampling have paved the way for improvements in
coastal sea-level research (e.g., Dieng et al., 2021; Prandi et al., 2021;
Dodet et al., 2020; Sanchez-Arcilla et al., 2021).</p>
      <p id="d1e139">Tide gauge stations operating along the North Sea coast provide high-quality
records of sea-level observations over a long period (Wahl et al., 2013).
Ponte et al. (2019), reviewing the state of the science of coastal sea-level
monitoring and prediction, outlined the importance of sea-level observations
for studying sea-level variability. However, tidal gauges do not provide
information about the basin-wide patterns of sea level. Furthermore, some of
these data are not continuous; different gauges do not always operate
simultaneously, and there are gaps in many of the records. Therefore, a
combination of numerical model results with tide gauge measurements would be
beneficial. A similar exercise was undertaken recently by Madsen et al. (2019) for the Baltic Sea and by Zhang et al. (2020) for the North Sea.
Zhang et al. (2020) used machine learning to reconstruct the sea-level
variability in the North Sea using observations from 19 coastal tide gauges
and data from numerical models. Notably, they concluded that a relatively
short-time record contains the most representative characteristics of
sea-level dynamics in the North Sea. While this was clear for tides, it was
not so obvious for changes in sea level caused by the atmosphere.</p>
      <p id="d1e143">The North Sea (Fig. 1a) is a shallow sea with an average depth of <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">90</mml:mn></mml:mrow></mml:math></inline-formula> m located at the European continental shelf. The dynamics of sea level in the North Sea, which is the region of our study, can be considered a coupled response to different forcings, such as barotropic tides, wind, and atmospheric pressure, as well as forcings from the open boundaries and rivers, including a thermohaline forcing. The coupling of the respective processes is, in most cases, nonlinear (Jacob and Stanev, 2017), therefore, one cannot easily identify the response to individual drivers in isolation. This happens when either oscillatory motions have large amplitudes, e.g., tidal currents approaching 1 m s<inline-formula><mml:math id="M2" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, or when wind-driven current is of the same order. Thus, there is a need to use methods tailored to detect and reproduce nonlinear dynamics. Nonlinear processes are difficult to predict, even with sophisticated models; therefore, one needs to identify situations in which predictions fail (Ponte et al., 2019). Furthermore, it is interesting to understand the reasons for the deviation in the model predictions from the observations. The detection of such situations in data from a network of tide gauges is the aim of the present study.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e170"><bold>(a)</bold> Location of tide gauge stations used in this study and M2 cotidal chart (M2 amplitudes (color scale) and phase lines (black isolines) reproduced from Jacob and Stanev, 2017). Additionally, snapshots of NEMO model water levels for two selected times are shown together with water
level residuals at tide gauge locations (black lines) and a plane fitted
linearly to these residuals (grey areas): <bold>(b)</bold> 7 January 2017, 16:00 UTC and <bold>(c)</bold> 11 January 2017, 20:00 UTC.</p></caption>
        <?xmltex \igopts{width=412.564961pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023-f01.jpg"/>

      </fig>

      <p id="d1e187">The spatial and temporal correlations of tide gauge data mirror the complex
sea-level dynamics in the North Sea (Fig. 2). First, tidal wave propagation is influenced by the topography of the North Sea. The north–south decrease in water depth shifts the central amphidromic point southwards (see Fig. 1a for the oscillation pattern of the semidiurnal M2 tide). Two additional amphidromic systems are generated as a result of the superposition of incident and reflected Kelvin waves and cross-shore Poincaré waves with centers in the north, off the Norwegian coast, and in the south, between Suffolk and Holland (Fig. 1a). The amplitude of the tidal wave increases towards the British coast. Off the Danish and Norwegian coasts, the amplitude of the wave is significantly smaller due to dissipation by bottom friction in the shallow southern part of the North Sea (Fig. 2a).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e192">Time versus position diagram series of <bold>(a)</bold> measured water levels, <bold>(b)</bold> water level residuals, <bold>(c)</bold> wind tendency  (defined as change in wind speed within 1 h), and <bold>(d)</bold> pressure anomaly for January 2017 at tide gauge positions.</p></caption>
        <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023-f02.png"/>

      </fig>

      <p id="d1e213">The circulation of the North Sea and thus the sea level is forced also by
the atmosphere through either wind stresses (Fig. 2c) or atmospheric
pressure gradients (Fig. 2d). Considering the length scales and depth of
the North Sea, the wind has a dominant effect. The prevailing westerly winds
result in a dominant cyclonic circulation. A reversal of circulation caused
by easterly winds seldom occurs (Stanev et al., 2019). For northwesterly and
southeasterly winds, circulation may stagnate. As shown by Jacob and Stanev (2017), the interaction between tidal and wind-driven currents is nonlinear in areas of strong currents, particularly in the German Bight, and the atmospheric variability affects the spring–neap variability more strongly
than the M2 tide. Additionally, shallow-water tides show significant small-scale spatial variability patterns in this region (Stanev et al., 2015b). Thus, in the southern North Sea, tidal forcing strongly impacts the residual circulation (Fig. 2b). In summary, the specific topography of the North Sea together with nonlinear effects lead to complex circulation
patterns that hamper sea-level prediction.</p>
      <p id="d1e217">Simple linear statistical methods, such as principal component analysis
(PCA), fail to predict nonlinear dynamics because they represent linear
combinations of mean states. Flinchem and Jay (2000) demonstrated that
wavelet transforms provide an approach that is well suited for tidal
phenomena that “deviate markedly from an assumed statistical stationarity
or exact periodicity inherent in traditional tidal methods” and that it can
also reveal features that harmonic analysis could not elucidate. In the same
context, neural networks (NNs) have been used for (extreme) tidal surge
prediction (French et al., 2017; Tayel and Oumeraci, 2015; and Bruneau et al., 2020). Similarly, Hieronymus et al. (2019) applied different machine learning techniques to
the regression problem of time series data from tide gauges, and Balogun and
Adebisi (2021) investigated the impact of different ocean–atmosphere
interactions on sea-level predictability using different NNs. However, all
these applications focus on data from single tide gauge stations.</p>
      <p id="d1e220">Horsburgh and Wilson (2007) proved the importance of spatial and temporal correlations
among tide gauge stations along the British coast for the distribution of
surge residuals. However, their linear model is only capable of describing
some of the possible interactions between tides and surges and was used to
demonstrate the existence of critical<?pagebreak page417?> spatiotemporal scales for surge
development and decay. Wenzel and Schröter (2010) used neural networks for the
reconstruction of monthly regional mean sea-level anomalies from 59 tide
gauges worldwide. Zhang et al. (2020) used generative adversarial networks to
reconstruct the sea-level variability in the North Sea using observations
from 19 coastal tide gauges and data from numerical models. Notably, they
concluded that a relatively short-term record contains the most
representative characteristics of sea-level dynamics in the North Sea. While
this was clear for tides, it was not so obvious for changes in sea level
caused by the atmosphere. Similarly, the deep learning approach to fuse
altimeter data with tide gauge data in the Mediterranean Sea was described
by Yang et al. (2021), while Nieves et al. (2021) used open ocean
temperatures to predict coastal sea-level variability via machine learning.</p>
      <?pagebreak page418?><p id="d1e223">In contrast to these applications, we will focus on the identification of
situations in which spatial correlations between tide gauge measurements
deviate greatly from the principal correlations. Usually, tide gauge
measurements in the North Sea show specific spatial correlations (changing
in time with the tide). However, in anomalous situations (e.g., localized
storms), these correlations may drastically change. We use autoassociative
neural networks (AANNs, Kramer, 1992) to detect such sea-level states.
Similar to PCA, the aim of this method is dimensionality reduction; however,
the concept of orthogonal vectors is expanded to principal curves. The
combination of nonlinear components best describing the variability in the
training data can be used to reconstruct the data. Thus, AANN provides a
nonlinear reconstruction model, and the reconstruction error is a measure of
how well the data are characterized. Large errors in the reconstruction of
data by the AANN represents situations in which the data do not belong to
the same distribution they were built from. Atmospheric conditions related
to such situations might aid further understanding and future developments
in sea-level prediction.</p>
      <p id="d1e226">The paper is structured as follows: in Sect. 2, we present observational and model data used throughout our study and introduce the concept of AANN. We then apply the AANN to the tide gauge array measurements in the North
Sea. In Sect. 3, we use AANN to detect anomalous events and examine the
dependence of identification of such events from the AANN training data
used. Two events are studied in detail, including their relationship with
the atmospheric conditions. This is followed by a discussion and
conclusions.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data and methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Observational and model data</title>
      <p id="d1e245">Observational sea-level data along the North Sea coast have been obtained
from the historical and near-real-time (NRT) dataset of the Copernicus
Marine Environment Monitoring Service (CMEMS). The observations were taken
from the respective in situ products for the northwest shelf area
(Copernicus Marine In Situ TAC Data Management Team, 2020; <ext-link xlink:href="https://doi.org/10.48670/moi-00045" ext-link-type="DOI">10.48670/moi-00045</ext-link>) with hourly resolution. The NRT in situ quality-controlled observations are updated hourly and distributed within approximately 24–48 h after acquisition. From these, we have chosen 14 gauge stations according to completeness of data time series. Their positions are shown in Fig. 1a. Time versus position diagrams of measured and detided (residual) water levels are shown in Fig. 2a, b. Figure 1a shows the propagation of the tidal wave along the North Sea coasts with water level amplitudes increasing southwards towards the English Channel. The slope of contours in Fig. 2 gives the speed of propagation of the tidal wave. The specific feature between the Cromer and Vlissingen stations identifies the small amphidromic system in front of the English Channel. This feature is not present in the detided data (Fig. 2b); the latter resembles the atmospheric forcing (Fig. 2c, d). In the presence of large gradients in wind tendency (Fig. 2c), the water surface tilts considerably (Fig. 1c).</p>
      <p id="d1e251">For the experiments discussed later in this study, we also use data from the
GCOAST (Geesthacht coupled coastal model system) circulation, wave, and ocean
model (Madec et al., 2017; Staneva et al., 2017, 2021; Bonaduce et al., 2020).
Wave–current interaction processes included in the model are momentum and
energy sea state-dependent fluxes, wave induced mixing, and Stokes–Coriolis
forcing. The model area covers the Baltic Sea, the Danish Straits, the North Sea, and part of the northeast Atlantic Ocean, with 3.5 km horizontal resolution. The data used in the present study are only for the North Sea region. The ocean circulation model is based on the Nucleus for European Modelling of the Ocean (NEMO v3.6). The wave model is WAM (cycle 4.7), a third-generation wave model that solves the action balance equation without any a priori restriction on the evolution of the spectrum. The two models are two-way coupled via the OASIS3-MCT version 2.0 coupler (Valcke et al., 2013). The NEMO setup used within the GCOAST system uses an explicit free-surface formulation; 50 hybrid <inline-formula><mml:math id="M3" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula>–<inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:msup><mml:mi>z</mml:mi><mml:mo>*</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> levels with partial cells
are used in the vertical. Atmospheric pressure and tidal potential are also
included in the model forcings (Egbert and Erofeeva, 2002). Daily river
run-off is based on river discharge datasets from the German Federal Maritime and Hydrographic Agency (Bundesamt für Seeschifffahrt und Hydrographie, BSH), Swedish Meteorological and Hydrological Institute (SMHI), and United Kingdom Meteorological Office (Met Office). Boundary conditions at the open boundaries (temperature, salinity, velocity, and sea level) are taken from the AMM7 model (O'Dea et al., 2012) distributed by the Copernicus Marine Environment and Monitoring Service. They have a temporal resolution of 1 h with a 7 km horizontal resolution. The model forcings for momentum and heat fluxes are computed using bulk aerodynamic formulae and hourly data from atmospheric reanalyses of the European Centre for Medium-Range Weather Forecasts (ERA5, Hersbach et al., 2020), the fifth generation of reanalysis of the ECMWF. We use ERA5 1-hourly products provided by Copernicus Climate Center Service (2021) available with 0.25<inline-formula><mml:math id="M5" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> horizontal resolutions for the atmospheric and wave parameters. Several studies have demonstrated the advantages of using the ERA5 reanalysis over its predecessor (ERA-INTERIM, e.g., Belmonte Rivas and Stoffelen, 2019).</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Autoassociative neural network</title>
      <p id="d1e289">Most environmental monitoring programs produce large sets of data, with the
tide gauge data network in the North Sea being among them (CMEMS global
ocean in situ near-real-time observations, 2020a;<?pagebreak page419?> <ext-link xlink:href="https://doi.org/10.48670/moi-00036" ext-link-type="DOI">10.48670/moi-00036</ext-link>). Although these sea-level data depend on a number of variables (tidal and atmospheric forcings together with bathymetry, river input, etc.), the number <inline-formula><mml:math id="M6" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> of tide gauges within the network is greater than the number of variables. The observed data are located within a subspace of the <inline-formula><mml:math id="M7" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>-dimensional data space and can thus be
compressed. Different machine learning techniques, such as the <inline-formula><mml:math id="M8" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>-nearest neighbors algorithm, ensemble-based methods, and support vector machine
(SVM) algorithms, are used to predict the posterior probabilities of a given
dataset and are optimal for data compression. The different techniques are
not equally well suited for detecting outliers, i.e., identifying whether a
given observation belongs to the same probability distribution. Outlier
detection in high dimensions, or without any assumptions about the
distribution function of the data, is very challenging. SVM algorithms work
well if training data are not contaminated by outliers. Ensemble and
<inline-formula><mml:math id="M9" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>-nearest neighbor methods perform well for multimodal datasets. Covariance estimators, in which category PCA also falls, degrade when the data are not unimodal.</p>
      <p id="d1e323">Autoassociative neural networks (AANNs) combine the robust performance of multimodal data with the geometric interpretability of PCA to identify these situations. An AANN is a reconstruction model based on a feed-forward neural network
(Kramer, 1992). In an AANN, the <inline-formula><mml:math id="M10" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>-dimensional input <inline-formula><mml:math id="M11" display="inline"><mml:mi mathvariant="bold-italic">x</mml:mi></mml:math></inline-formula> is mapped onto itself (<inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo mathvariant="bold">′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>) with a data compression step in between: the number of neurons in at least one hidden layer in an AANN is less than the dimension <inline-formula><mml:math id="M13" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> of the input and output vectors <inline-formula><mml:math id="M14" display="inline"><mml:mi mathvariant="bold-italic">x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo mathvariant="bold">′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>. This layer is called the bottleneck layer and is the key component of an AANN (Fig. 3a). It provides data compression of the input with powerful feature extraction capabilities. The mapping part <inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> compresses the information of the <inline-formula><mml:math id="M17" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>-dimensional vector to a smaller dimension subspace vector <inline-formula><mml:math id="M18" display="inline"><mml:mi mathvariant="bold-italic">p</mml:mi></mml:math></inline-formula>, whereas the demapping part <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo mathvariant="bold">′</mml:mo></mml:msup><mml:mo>=</mml:mo><mml:mi mathvariant="normal">d</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">p</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> uses compressed information to regenerate the original <inline-formula><mml:math id="M20" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>-dimensional vector.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e435"><bold>(a)</bold> Autoassociative NN with bottleneck: the input is mapped by <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:mi mathvariant="bold-italic">p</mml:mi><mml:mo>=</mml:mo><mml:mi>m</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> onto a lower dimensional space (<inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:mtext>dim</mml:mtext><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">p</mml:mi><mml:mo>)</mml:mo><mml:mo>&lt;</mml:mo><mml:mtext>dim</mml:mtext><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>) and is approximately reconstructed by the demapping NN part <inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mo mathvariant="bold">′</mml:mo></mml:msup><mml:mo>=</mml:mo><mml:mi mathvariant="normal">d</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">p</mml:mi><mml:mo>)</mml:mo><mml:mo>≈</mml:mo><mml:mi mathvariant="bold-italic">x</mml:mi></mml:mrow></mml:math></inline-formula>. <bold>(b)</bold> Error measure from the training sample versus the number of neurons in the AANN “bottleneck” layer using the 2016/17 North Sea water level data from the 14 tide gauge stations (see Fig. 1).</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023-f03.png"/>

        </fig>

      <p id="d1e517">In the mapping part, the (nonlinear) correlations/functional relations
existing among the input variables (here, the spatial correlations) are
taken advantage of. Thus, an AANN can be considered to perform a nonlinear
generalization of the PCA (nonlinear principal component analysis, NLPCA; Kramer, 1991). Similar to PCA, NLPCA can also serve important purposes,
e.g., filtering noisy data, feature extraction, data compression, outliers
and novelty detection (Mori et al., 2016).</p>
      <p id="d1e520">During training, the AANN constructs a model that captures the posterior
probability distribution of a given dataset.</p>
      <p id="d1e523">At the beginning of the training, the outcome of the NN will differ largely
from the target output. The mean squared relative error per neuron <inline-formula><mml:math id="M24" display="inline"><mml:mi>e</mml:mi></mml:math></inline-formula> is iteratively minimized during the training by backpropagating the error through the NN and adjusting free parameters according to a gradient descent scheme:
            <disp-formula id="Ch1.Ex1"><mml:math id="M25" display="block"><mml:mtable rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mi>e</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mi>N</mml:mi></mml:mfrac></mml:mstyle><mml:msubsup><mml:mo>∑</mml:mo><mml:mrow><mml:mi mathvariant="normal">tr</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:msubsup><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">tr</mml:mi></mml:msub><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:msub><mml:mi>e</mml:mi><mml:mi mathvariant="normal">tr</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mi>n</mml:mi></mml:mfrac></mml:mstyle><mml:msubsup><mml:mo>∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:msubsup><mml:mo mathsize="2.5em">(</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>x</mml:mi><mml:msub><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup><mml:mi>i</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mo>max⁡</mml:mo><mml:mfenced close=")" open="("><mml:mrow><mml:msubsup><mml:mi>x</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">tr</mml:mi></mml:msubsup></mml:mrow></mml:mfenced><mml:mo>-</mml:mo><mml:mo>min⁡</mml:mo><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>x</mml:mi><mml:msubsup><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup><mml:mi>i</mml:mi><mml:mi mathvariant="normal">tr</mml:mi></mml:msubsup></mml:mrow></mml:mfenced><mml:mo>,</mml:mo><mml:mtext>tr</mml:mtext><mml:mo>∈</mml:mo><mml:mfenced open="[" close="]"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mi>N</mml:mi></mml:mrow></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle><mml:msup><mml:mo mathsize="2.5em">)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
          where <inline-formula><mml:math id="M26" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> is the number of (training) input/output data pairs.</p>
      <p id="d1e681">An important step in the construction of an appropriate AANN is the choice
of the number of neurons in the bottleneck layer, i.e., to determine the
dimension of the subspace <inline-formula><mml:math id="M27" display="inline"><mml:mi mathvariant="bold-italic">p</mml:mi></mml:math></inline-formula>. The choice is based on the reconstruction abilities of the network: the overall reconstruction error of
the AANN decreases with an increasing number of neurons in the bottleneck
layer. However, if the number of bottleneck neurons equals the intrinsic
dimensionality, a further increase leads to “overfitting” of the AANN, i.e., learning stochastic variations in the dataset rather than the underlying functions. As a result, the decrease in the overall error flattens (Fig. 3b).</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Application of AANN to the North Sea water level from tide
gauges</title>
      <p id="d1e699">The proposed scheme was applied to data from 14 (<inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:mtext>dim</mml:mtext><mml:mo>(</mml:mo><mml:mi>n</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mn mathvariant="normal">14</mml:mn></mml:mrow></mml:math></inline-formula>) tide
gauges along the North Sea coast (Sect. 2.1). Data from 2016/17 were used
to train the AANNs; data from 2018 were retained as an independent testing
set. A 2-year training period was assumed to be long enough to capture the
essential spatial correlations among observations at different gauges well.
Thus, any dominant factor affecting the interrelationship between observations from individual stations (bathymetry, the distance between
stations, dominant winds, and atmospheric pressure, etc.) should be reflected
by the AANN. The choice of tide gauge locations was a compromise between
spatial coverage and data availability (since missing data from single gauge
stations were not filled, e.g., by interpolation, and thus resulted in data
loss). We applied no further preprocessing or quality control to the tide
gauge data.</p>
      <p id="d1e720">A sequence of AANNs with an increasing number of neurons in the bottleneck
layer was trained to map the 14 water levels onto themselves. In Fig. 3b,
the relative reconstruction error <inline-formula><mml:math id="M29" display="inline"><mml:mi>e</mml:mi></mml:math></inline-formula> for all training data is plotted versus the number of neurons in the bottleneck layer. Error decreases with an increasing number of bottleneck neurons; the decrease starts to flatten at seven neurons (<inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:mtext>dim</mml:mtext><mml:mo>(</mml:mo><mml:mi mathvariant="bold-italic">p</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:math></inline-formula>) in the bottleneck layer. Therefore, we decided to use seven bottleneck neurons and refer to this as AANN_ref (reference AANN).</p>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Quality of AANN analysis</title>
      <p id="d1e756">The performance of the AANN_ref is shown in Fig. 4. The scatterplots are used to compare the modeled vs. observed sea-level data. The distribution for the training phase (Fig. 4a) closely follows the bisectrix and is very narrow. The standard deviation between the observed and AANN<?pagebreak page420?> reconstructed sea-level data is approximately 10 cm (Fig. 4c). For the testing phase (Fig. 4b, d), the agreement between the observations and modeled data is almost as good as that for the training phase; however, some scatter is also clearly seen. Parts of this disagreement, with errors above the 99.9th percentile during the training phase, are marked in red and indicate possible candidates for anomalous situations, which will be further analyzed. The distribution of errors is non-Gaussian during training and testing (Fig. 4c, d). The long tail of the error histogram shows data where the reconstruction by AANN failed and where anomalous correlations among tide gauges are expected.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e761">Performance of the reference AANN <bold>(a–d)</bold> and of the PCA <bold>(e–h)</bold> in reconstructing sea-level data during the training <bold>(a, c, e, g)</bold> and testing <bold>(b, d, f, h)</bold> period. Red points indicate matchups with an absolute reconstruction error <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">50.4</mml:mn></mml:mrow></mml:math></inline-formula> cm. This limit was derived from the
0.01 % of training data with highest reconstruction error for the reference AANN. Histograms <bold>(c, d, g, h)</bold> show the respective distributions of squared relative reconstruction errors <inline-formula><mml:math id="M32" display="inline"><mml:mi>e</mml:mi></mml:math></inline-formula>. The numbers are the mean error and standard deviation of the reconstruction. Insets show the tail of the distributions, containing possible candidates for anomalous sea states. Additionally, absolute mean errors and standard deviations are given.</p></caption>
          <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023-f04.png"/>

        </fig>

      <p id="d1e803">The non-Gaussian nature of the error distribution demonstrates the
capability of the AANN to capture complex (usually nonlinear) processes.
This is the fundamental difference from the case when PCA (using seven PCs,
analogous to the number of bottleneck neurons in AANN_ref) is
used to reconstruct the observed data (Fig. 4e–h). In PCA, the results
have approximately 3.5 times higher standard deviations. PCA here leads to a
short-tailed Gaussian error distribution (Fig. 4g, h), making it
unsuitable for the desired task. Because the non-Gaussian distribution is a
typical characteristic of nonlinear processes, and because linear methods
(PCA) do not capture it, we conclude that the above comparison gives a clear
demonstration of the power of the AANN method used in the present study to
handle nonlinearities. Outliers are usually in the tail of the distribution,
and their identification requires using nonlinear reconstruction methods.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Anomalous sea levels and their relationship with atmospheric
conditions</title>
      <p id="d1e815">To isolate events that strongly affect the spatial correlations among tide
gauges, further constraints are needed. High values of AANN_ref reconstruction errors might originate from events on small scales, such
as ocean response to wind gusts, as well as the erroneous measurement of a
single tide gauge. From the analysis of the training period, we postulate an
ocean state as anomalous when the <italic>error e exceeds 0.035 (see Fig. 4c, d) for at least three gauges simultaneously for at least 3 h</italic>.</p>
      <p id="d1e821">To exclude the dependence of identification of such extreme events from the
data used, we trained alternative AANNs based on the following datasets:
<list list-type="bullet"><list-item>
      <p id="d1e826">trained with data extracted at the closest positions of gauge stations from the CMEMS operational model AMM15 (AANN_NEMO);</p></list-item><list-item>
      <p id="d1e830">trained with a subset of gauge data from only 10 stations (with Dover, Oostende, Vlissingen, and Europlatform in the southwest corner of the North Sea excluded) (AANN_less); and</p></list-item><list-item>
      <p id="d1e834">trained with detided data from the 14 gauge stations (AANN_resid). Software package T-TIDE (Pawlowicz et al., 2002) was used for this purpose.</p></list-item></list>
As for AANN_ref, training data span the 2-year period 2016/17 and data from 2018 were kept for validation.</p>
      <p id="d1e838">The first additional network AANN_NEMO allows an intercomparison between observations and simulations. If the agreement is good, spatial data from the operational model will enable the analysis of horizontal patterns associated with the identified events. The second network, AANN_less, identifies the possible occurrence of anomalous events in the southwestern North Sea area. This area is known to be dominated by a small amphidromic system (Fig. 1a) and is characterized by its complex dynamics and high amplitudes of tidal oscillations. The third network, AANN_resid, reveals how strongly anomalous events are associated with the basic tidal dynamics, which are removed here.</p>
      <p id="d1e841">The error distributions of AANN_less, AANN_resid, and AANN_NEMO are similar to those of AANN_ref. The tail of the AANN_NEMO error distribution is shortened, making modeling data less suitable for novelty
detection (see<?pagebreak page421?> Fig. 5c, d). A comparison of AANN_NEMO and AANN_ref errors is shown in Fig. 6. Anomalous situations detected with AANN_ref (4, 11–14 January 2017) reflect themselves in large (exceeding 25 cm) AANN_NEMO errors but not necessarily vice versa.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e847">Same as Fig. 4 but for AANN_NEMO trained on NEMO
modeled sea-level data.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023-f05.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e858">Time versus position diagrams of differences between <bold>(a)</bold> measured
water levels and AANN_ref emulated ones and between <bold>(b)</bold> NEMO
modeled and AANN_NEMO emulated ones for January 2017.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023-f06.jpg"/>

      </fig>

      <p id="d1e873">The proposed criterion was tested on the reference model AANN_ref for the 2018 testing period. Several anomalous sea states were detected (Table 1). Events in the winter months occur more than twice as often as in other  seasons. Afterwards, it was verified whether a specific event could be observed with AANNs trained on alternative datasets (see Table 1). Due to
the short-tailed error distribution, all events can be detected with AANN_NEMO (but as a stand-alone method, it gives a larger number of false alarms). Events from autumn and winter are also detected with the alternative AANNs (AANN_resid and AANN_less). This does not apply to spring and summer, where some events are not detected with AANN_less and/or by
AANN_resid.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e879">Overview of the number of anomalous sea states detected by the
alternative training dataset AANN and the reference model
AANN_ref (values in bold) approaches during the 2018 testing phase.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="6">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="center"/>
     <oasis:colspec colnum="4" colname="col4" align="center"/>
     <oasis:colspec colnum="5" colname="col5" align="center"/>
     <oasis:colspec colnum="6" colname="col6" align="center"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Training  dataset</oasis:entry>
         <oasis:entry colname="col3">Spring</oasis:entry>
         <oasis:entry colname="col4">Summer</oasis:entry>
         <oasis:entry colname="col5">Autumn</oasis:entry>
         <oasis:entry colname="col6">Winter</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">(MAM)</oasis:entry>
         <oasis:entry colname="col4">(JJA)</oasis:entry>
         <oasis:entry colname="col5">(SON)</oasis:entry>
         <oasis:entry colname="col6">(DJF)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">AANN_NEMO</oasis:entry>
         <oasis:entry colname="col2">NEMO model (14 data points)</oasis:entry>
         <oasis:entry colname="col3">2</oasis:entry>
         <oasis:entry colname="col4">2</oasis:entry>
         <oasis:entry colname="col5">6</oasis:entry>
         <oasis:entry colname="col6">13</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">AANN_less</oasis:entry>
         <oasis:entry colname="col2">Tide gauge data (raw, 10 gauges)</oasis:entry>
         <oasis:entry colname="col3">1</oasis:entry>
         <oasis:entry colname="col4">0</oasis:entry>
         <oasis:entry colname="col5">6</oasis:entry>
         <oasis:entry colname="col6">13</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">AANN_resid</oasis:entry>
         <oasis:entry colname="col2">Tide gauge data (detided, 14 gauges)</oasis:entry>
         <oasis:entry colname="col3">1</oasis:entry>
         <oasis:entry colname="col4">1</oasis:entry>
         <oasis:entry colname="col5">6</oasis:entry>
         <oasis:entry colname="col6">13</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><bold>AANN_ref</bold></oasis:entry>
         <oasis:entry colname="col2"><bold>Tide gauge data (raw, 14 gauges)</bold></oasis:entry>
         <oasis:entry colname="col3"><bold>2</bold></oasis:entry>
         <oasis:entry colname="col4"><bold>2</bold></oasis:entry>
         <oasis:entry colname="col5"><bold>6</bold></oasis:entry>
         <oasis:entry colname="col6"><bold>13</bold></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e1044">Snapshots show the wind <bold>(a)</bold> and pressure <bold>(b)</bold> fields at the time of the largest wind tendency occurrence (6 June 2017, 12:00 UTC). Relatedly, the snapshot <bold>(c)</bold> shows NEMO ssh at the time of the largest AANN error (6 June 2017, 22:00 UTC) together with tide gauge residuals (black lines). The grey area shows the orientation of a plane fitted linearly to these residuals.</p></caption>
        <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023-f07.jpg"/>

      </fig>

      <?pagebreak page422?><p id="d1e1062">In the following, we will analyze two such events: the first event from June
2017 (low pressure “Heinrich”) was chosen since it was detected by AANN_resid but not by AANN_less (Figs. 7 and, 8c, d). This atmospheric system brought some unseasonably wet and windy weather from France to the British southeast coast through the Channel. The rain was accompanied by very strong westerly winds (<inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">15</mml:mn></mml:mrow></mml:math></inline-formula> m s<inline-formula><mml:math id="M34" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), with gusts of 20–25 m s<inline-formula><mml:math id="M35" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> around the coast of England and Wales (see Figs. 7a, b and 8c, d). As a result, the measured sea level (Fig. 8a) exceeded the AANN_ref modeled sea level over several hours along the western Dutch coast and southeastern British coast (Fig. 9a). The AANN_ref and AANN_NEMO (Fig. 9b) errors are largest at Oostende, where the measured low tide is higher than expected by the AANNs. The occurrence of the largest error shifts to Dover for AANN_resid and to Den Helder for PCA (Fig. 9e, f). The NEMO model error (Fig. 9c) is the largest for Vlissingen, where it under- and overestimates the measured values for high and low tides, respectively. Consistently, AANN_less does not detect the event (Fig. 9d), indicating its origin in anomalous spatial correlations among gauges around the small amphidromic system. Thus, the specific forcing resulted in a localized (exceptional) increase in sea level at gauge station Den Helder. The snapshot in Fig. 7c visualizes this finding at the time the AANN largest errors occurred, 10 h after the wind tendency.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e1101">Time versus position diagrams of measured tide gauge data <bold>(a)</bold>, its
residuals <bold>(b)</bold>, and atmospheric forcing (ERA5 data, wind tendency <bold>(c)</bold>, and pressure anomaly <bold>(d)</bold>) for 1–15 June 2017.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023-f08.jpg"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><?xmltex \currentcnt{9}?><?xmltex \def\figurename{Figure}?><label>Figure 9</label><caption><p id="d1e1124">Time versus positions diagrams of different reconstruction errors
with respect to measured (detided) and NEMO modeled tide gauge data for
1–15 June 2017: <bold>(a)</bold> AANN_ref, <bold>(b)</bold> AANN_nemo
(trained on modeled data), <bold>(c)</bold> NEMO model, <bold>(d)</bold> AANN_less (without 4 stations close to the small amphidromic system), <bold>(e)</bold> AANN_resid (trained on water level residuals), and <bold>(f)</bold> using PCA, respectively.</p></caption>
        <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023-f09.jpg"/>

      </fig>

      <?pagebreak page423?><p id="d1e1152">As a second example, a typical winter storm was chosen: the deep depression
“Burglind” (Figs. 10a, b and 11c, d), which was associated with high wind
speeds (up to 20 m s<inline-formula><mml:math id="M36" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) along the English and the Dutch coasts but also with large gradients in the wind field (Fig. 7a) with gusts exceeding 33 m s<inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in England and Wales. The storm track passed over Ireland, crossed the United Kingdom, and then moved over central Europe and dissipated.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F10" specific-use="star"><?xmltex \currentcnt{10}?><?xmltex \def\figurename{Figure}?><label>Figure 10</label><caption><p id="d1e1182">Same as Fig. 7, but at the time of the largest wind tendency occurrence (3 January 2018, 06:00 UTC) and largest AANN reconstruction error
(3 January 2018, 13:00 UTC) during storm “Burglind”.</p></caption>
        <?xmltex \igopts{width=384.112205pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023-f10.jpg"/>

      </fig>

      <?xmltex \floatpos{p}?><fig id="Ch1.F11" specific-use="star"><?xmltex \currentcnt{11}?><?xmltex \def\figurename{Figure}?><label>Figure 11</label><caption><p id="d1e1193">Same as Fig. 8, but for 1–15 January 2018.</p></caption>
        <?xmltex \igopts{width=412.564961pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023-f11.jpg"/>

      </fig>

      <p id="d1e1202">As a result, the measured tide gauge values exceeded the AANN_ref, AANN_NEMO, and AANN_less values at stations along the southern English and Dutch coasts (Fig. 12a, b, d). Exceptions are Lowestoft and Cromer in the “shadow” of the cyclone. The NEMO model results (Fig. 12c) show good agreement during high tide, especially along the Scottish coast, but tend to overestimate the low tide values, especially along the Dutch coast.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12" specific-use="star"><?xmltex \currentcnt{12}?><?xmltex \def\figurename{Figure}?><label>Figure 12</label><caption><p id="d1e1207">Same as Fig. 9, but for 1–15 January 2018.</p></caption>
        <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://nhess.copernicus.org/articles/23/415/2023/nhess-23-415-2023-f12.jpg"/>

      </fig>

      <p id="d1e1216">AANN_resid and PCA (Fig. 12e, f) also detect the event. However, here, stations along the Dutch coast have the largest reconstruction errors (i.e., stations with the highest water level residuals, see Fig. 11b). The snapshot in Fig. 10c visualizes water level residuals at the time of the largest AANN errors, which occurred with a 7 h delay to wind tendency.</p>
      <?pagebreak page425?><p id="d1e1220">On either occasion, a typical time delay of 5 to 15 h between large tendencies in wind forcing and large reconstruction errors is observed, supporting the assumption that the atmosphere plays a key role in the
detected events. However, their occurrence cannot be directly linked to atmospheric variables, such as large tendencies in the wind forcing. These
tendencies occur often but seldom result in such anomalous correlations
between tide gauge measurements.</p>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Conclusions</title>
      <p id="d1e1231">We presented a tool for detecting anomalous water levels from a network of tide gauges in the North Sea using AANN. Strong spatial correlations between gauges allow for a reconstruction model in a lower dimensional subspace. Combining a threshold value for reconstruction error with the requirement of its occurrence at three different gauges for at least three hours has been shown to be a valuable filter for such events. For the two events discussed in detail, atmospheric conditions showed high wind tendencies and pressure anomalies, with the accumulation of water masses in specific areas. Thus, the resultant sea states are assumed to be related to nonlinear interactions among the various atmospheric and oceanic forcings. Further analysis is needed to develop a deeper understanding of the underlying processes. Ultimately, this understanding might improve numerical sea-level predictions. The AANN reveals an intrinsic dimensionality of <inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:math></inline-formula>. Evident variable candidates that could be involved in further studies
include location (latitude/longitude), time, wind tendency, pressure anomaly,
and information on water currents.</p>
      <p id="d1e1246">In addition, the tool offers an inexpensive opportunity to monitor the tidal
gauge array. The difference between using raw and detided data as input to
the model was marginal. Thus, no further data preprocessing is needed. The
AANN model reacts sensitively to the choice of tide gauge locations:
AANN_less, where stations around the small amphidromic system were removed from the training data, was not able to identify events resulting from storms along the channel.</p>
      <p id="d1e1249">The linear PCA reconstruction method reveals a high rate of false positive
alarms, which indicates a multimodal probability distribution of the
sea-level data. The detection of some of these events might fail for AANN_NEMO. This finding substantiates the hypothesis that AANN is able to detect situations under which model physics need further improvement.</p>
      <p id="d1e1252">The proposed method can be adapted easily to any tide gauge array. However,
the intrinsic dimensionality of the constructed AANN might differ, as well
as the involved forcings and underlying processes.</p>
</sec>

      
      </body>
    <back><notes notes-type="codeavailability"><title>Code availability</title>

      <p id="d1e1259">The neural net program (Schiller, 2000) used in this study is available upon request to the corresponding author.</p>
  </notes><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e1265">Tide gauge data used in this study are available at <ext-link xlink:href="https://doi.org/10.48670/moi-00045" ext-link-type="DOI">10.48670/moi-00045</ext-link> (Copernicus Marine In Situ TAC Data Management Team, 2020). The atmospheric data can downloaded from Climate Data Store (<uri>https://cds.climate.copernicus.eu</uri>, last access: 20 July 2021). The outputs of NEMO model simulations (in NetCDF format) are available upon request to the corresponding author.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e1277">KW, EVS, and JS conceived the concept and methodology of the presented idea. The authors discussed the<?pagebreak page426?> results and have all contributed to the
original draft preparation and its reviewing. JS supervised the project.
KW designed the computational framework and analyzed the data.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e1283">The contact author has declared that none of the authors has any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e1289">Publisher’s note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><notes notes-type="sistatement"><title>Special issue statement</title>

      <p id="d1e1296">This article is part of the special issue “Coastal hazards and hydro-meteorological extremes”. It is not associated with a conference.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e1302">We acknowledge the Cluster of Excellence EXC20 2037 “Climate, Climatic Change, and Society” (CLICCS) (project no. 390683824). Emil V. Stanev acknowledges the EU H2020 project DOORS (grant no. 101000518). Joanna Staneva acknowledges funding from the European Green Deal project “Large scale RESToration of COASTal ecosystems through rivers to sea connectivity” (REST-COAST) (grant no. 101037097). Kathrin Wahle gratefully acknowledges funding from the EU H2020 project IMMERSE (grant no. 821926). We would like to thank Sebastian Grayek for providing NEMO model output data.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e1307">This research has been supported by the European Green Deal project “Large scale RESToration of COASTal ecosystems through
rivers to sea connectivity” (REST COAST, grant no. 101037097), the EU
H2020 project IMMERSE (grant no. 821926), the Cluster of Excellence EXC20 2037 “Climate, Climatic Change, and Society” (CLICCS) (project no. 390683824), and the EU H2020 project DOORS (grant no. 101000518). <?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
The article processing charges for this open-access <?xmltex \notforhtml{\newline}?>publication were covered by the Helmholtz-Zentrum Hereon.</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e1318">This paper was edited by Piero Lionello and reviewed by two anonymous referees.</p>
  </notes><ref-list>
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